钢件表面强化过程中接触相互作用的仿真模型

K. Holenko, V. Dytyniuk, M. Dykha
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引用次数: 0

摘要

在钢件表面强化过程中,应力-应变状态对解释强化的物理过程、形成接触面积的尺寸具有决定性作用。接触参数的解析依赖性是相当近似的。本文基于Ansys软件,建立了一个截形环面与圆柱体接触的仿真模型,用于模拟硬质合金刀具挤压钢质工件-圆柱体的动力学过程。为了确定卸荷后的最大应力水平、应力分布和残余应力量,进行了4秒的实验。夹紧力主要作用在弹性变形区。结果表明:接触点的应力分布不均匀,在接触点的中心处应力最大值为1082 MPa;改变载荷方向后,接触片中心出现了0.00311 μm量级的微小残余变形。这表明在一个小的接触区域上有弹性区域的破坏,它不影响应力分布的一般性质,并且可以在精加工过程中消除。应力状态的模拟结果与观察到的材料在热应力和功率应力作用下的结构变化进行了对比。应力峰值在200 μm处形成,这是造成显微硬度最大值的主要原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Simulation model of contact interaction during surface strengthening of steel parts
In the processes of surface strengthening of steel parts, the stress-strain state is decisive for explaining the physical processes of strengthening, forming the dimensions of the contact area. Analytical dependences of contact parameters are quite approximate. In this work, based on the Ansys software complex, a simulated model of the contact of a truncated torus with a cylinder is proposed, which demonstrates the kinetics of the process of pressing a hard alloy tool into a steel workpiece - a cylinder. The experiment was conducted for 4 seconds in order to determine the maximum level of stresses, the distribution of stresses and the amount of residual stresses after removing the load. The clamping force was applied mainly in the zone of elastic deformations. The results showed an uneven stress distribution with a maximum in the center of the contact spot of 1082 MPa. After changing the load direction, small residual deformations at the level of 0.00311 μm were observed in the center of the contact patch. This indicates a violation of the elastic region on a small contact area, which does not affect the general nature of the stress distribution and can be removed during the finishing process. The results of simulation of the stressed state are used for the correlation with the observed structural changes of the material during the action of thermal and power stresses. The stress peak was formed at a distance of 200 μm, which contributes to the formation of maximum values of microhardness at this depth.
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